2011
DOI: 10.1016/j.nima.2011.05.072
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Radiative regime of linear colliders, high repetetion rate free electron lasers and associated accelerating structures

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Cited by 3 publications
(2 citation statements)
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“…However, in both of these pioneering experiments the energy gain was limited by the energy carried by the driver and the propagation length of the driver in the plasma (< 1 m). The laser pulse and electron bunch driver schemes therefore require staging [4,5]; i.e., the stacking of many 10 − 25 GeV acceleration, or plasma, stages to reach the ∼ 1 TeV energy per particle or equivalently ∼ 2 kJ of energy in ∼ 2 × 10 10 electrons and positrons. The AWAKE scheme avoids these propagation-length and energy limitations by using a proton bunch to drive the wakefields.…”
Section: Proton-driven Plasma Wakefield Accelerationmentioning
confidence: 99%
“…However, in both of these pioneering experiments the energy gain was limited by the energy carried by the driver and the propagation length of the driver in the plasma (< 1 m). The laser pulse and electron bunch driver schemes therefore require staging [4,5]; i.e., the stacking of many 10 − 25 GeV acceleration, or plasma, stages to reach the ∼ 1 TeV energy per particle or equivalently ∼ 2 kJ of energy in ∼ 2 × 10 10 electrons and positrons. The AWAKE scheme avoids these propagation-length and energy limitations by using a proton bunch to drive the wakefields.…”
Section: Proton-driven Plasma Wakefield Accelerationmentioning
confidence: 99%
“…However, in both of these pioneering experiments the energy gain was limited by the energy carried by the driver (∼ 100 J) and the propagation length of the driver in the plasma (< 1 m). The laser pulse and electron bunch driver schemes therefore require staging [8,9], i.e. the stacking of many 10 − 25 GeV acceleration, or plasma, stages to reach the ∼ 1 TeV energy per particle or equivalently ∼ 2 kJ of energy in ∼ 2 × 10 10 electrons and positrons.…”
Section: Introductionmentioning
confidence: 99%